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Application of calcite, Mg-calcite, and dolomite as Raman pressure sensors for high-pressure, high-temperature studies

机译:方解石,Mg-方解石和白云岩的应用作为拉曼压力传感器,高压,高温研究

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摘要

The Raman spectra of calcite, Mg-calcite, and dolomite were measured under ambient and high pressure-temperature (P-T) conditions using a hydrothermal diamond anvil cell, for the purpose of developing new pressure sensors suited for experiments investigating the physicochemical properties of carbonate minerals. By fitting the Raman vibrational frequencies as functions of pressure and temperature, pressure (P, in MPa) can be determined from relative frequency shifts (in cm(-1)) of the symmetric stretching (nu(1)) and librational (nu(L)) lattice vibrations of calcite: P = 229(1) x (nu(1 calcite, HP) - nu(1 calcite, ref)), P = 162(1) x (nu(L calcite, HP) - nu(L calcite, ref)), or from the translational (nu(T)) and librational (nu(L)) lattice vibrations of dolomite: P = 371(3) x [(nu(L dolomite, HP) - nu(T dolomite, HP)) - (nu(L dolomite, ref) - nu(T dolomite, ref))], where nu(ref) is the value under ambient P-T conditions. Under elevated temperatures, correction for the effect of temperature (T, in degrees C) on the Raman frequency shifts can be accomplished through nu(1 calcite, HT) = nu(1 calcite, ref) - 6.8(5) x 10(-6) x T-2-0.0051(3) x T + 0.12, nu(L calcite, HT) = nu(L calcite, ref) - 1.07(12) x 10(-5) x T-2-0.00341(7) x T + 0.76, nu(L dolomite, HT) - nu(T dolomite, HT) = (nu(L dolomite, ref) - nu(T dolomite, ref)) - 0.0198(3) x T + 0.45. Application of the calcite and dolomite Raman pressure sensors should be made on condition that no phase transitions or breakdown reactions occur under high P-T conditions, with errors of +/- 50 MPa and +/- 5% at pressures below and above 1.0 GPa, respectively. Results from an additional experiment showed that pressures determined using alternate Raman pressure calibration methods were self-consistent and in excellent agreement with the results determined using the nu(1) Raman peak shifts of aragonite.
机译:通过水热金刚石砧座细胞在环境和高压 - 温度(Pt)条件下测量方解石,Mg-Calimite和白云石的拉曼光谱,以开发适用于研究碳酸盐矿物的物理化学性质的实验的新压力传感器。通过将拉曼振动频率拟合作为压力和温度的函数,可以从对称拉伸(NU(1))和兼容(NU( l))方解石的晶格振动:p = 229(1)x(nu(1方解石,hp) - nu(1方解石,ref)),p = 162(1)x(nu(l Calcite,Hp) - nu (L Calipite,Ref)),或来自平移(NU(T))和扩展(NU(L))多米石的晶格振动:p = 371(3)x [(nu(l dolomite,hp) - nu( T白云岩,HP)) - (Nu(L Dolomite,Ref) - Nu(T Dolomite,Ref))],Nu(Ref)是环境PT条件下的值。在升高的温度下,通过Nu(1方解石,HT)= NU(1方解石,REF) - 6.8(5)×10( - 6)X T-2-0.0051(3)X T + 0.12,NU(L Calipite,HT)= Nu(L Calcite,Ref) - 1.07(12)x 10(-5)x T-2-0.00341(7 )X T + 0.76,Nu(L Dolomite,HT) - Nu(T Dolomite,HT)=(NU(L Dolomite,Ref) - Nu(T Dolomite,REF)) - 0.0198(3)x T + 0.45。应在高PT条件下不发生相移转变或分解反应的情况下进行方解石和白云石拉曼压力传感器的应用,分别在低于1.0GPa的压力下+/- 50MPa和+/- 5%的误差。另外的实验结果表明,使用交替拉曼压力校准方法测定的压力是自我一致的,并且与使用基范围的Nu(1)拉曼峰值峰值测定的结果非常吻合。

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